Optical information reproducing system with a reading beam having frequency components of N wavelengths corresponding to four times the N depths to a row of pits

Abstract

Disclosed is an optical disk having at least one pit in each of unit areas continuously provided in a circumferential direction of the disk, said pit having a depth of at least one of n depths (n: an integer equal to or greater than 2). Also disclosed is an information reproducing method of reproducing pit information from such an optical disk. This method comprises the steps of irradiating a read beam having frequency components of n wavelengths corresponding to four times the n depths to a row of the unit areas, and acquiring pit information based on an intensity distribution in a plane perpendicular to the optical axis of a reflected beam from the row of unit areas.

Description

This is a divisional of application Ser. No. 08/019,271 filed Feb. 18, 1993, now abandoned as of Aug. 18, 1995.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to an optical disk and an optical-disk information reproducing method of reproducing recorded information from the optical disk.

2. Description of the Related Art

Conventional optical disks, such as compact disks (CDs) or video disks (VDs), have pit information recorded in the form of the presence or absence of pits with a given depth and length. The pit information is reproduced with a read beam of a single wavelength.

The amount of information recordable on such an optical disk is restricted by the sizes of the pits and the read beam spot (the wavelength λ and the number of apertures NA of the objective lens), so that the recording density has reached the maximum level at present.

It is therefore difficult to further improve the recording density of information on an optical disk.

SUMMARY OF THE INVENTION

Accordingly, it is an object of the present invention to provide an optical disk designed to improve the information recording density, and an optical-disk information reproducing method of reproducing pit information from the optical disk.

To achieve this object, an optical disk according to the present invention has pit information recorded by setting the depth of at least one of the pits provided in individual unit areas continuously provided in the circumferential direction to one of n types of depths (n: an integer equal to or greater than 2).

An optical-disk information reproducing method embodying the present invention irradiates a read beam including frequency components of wavelengths respectively equal to four times n types of depths of pits on an optical disk and acquires pit information based on a reflected beam from each of the unit areas.

According to the information reproducing method of this invention, pit information is acquired by the level of a difference signal representing the difference between received light signals from a plurality of receiving surfaces perpendicular to the optical axis of the reflected beam of each unit area on an optical disk. In addition, the information about the presence of divided pits for each divided area or arrangement information is acquired by comparing the levels of sum signals of received light signals from a plurality of receiving surfaces perpendicular to the optical axis of the reflected beam.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is an exemplary diagram illustrating the arrangement of pits on the recording surface of an optical disk according to a first embodiment of the present invention;

FIGS. 2A and 2B respectively present a cross section showing the optical system of a pickup which picks up information from the optical disk in FIG. 1 and a circuit diagram showing the electric circuit of this pickup;

FIG. 3 presents a characteristic diagram showing the relationship between the wavelength of a read beam to be irradiated on pits having a given depth and the level of a difference signal;

FIG. 4 is an exemplary diagram illustrating the arrangement of pits on the recording surface of an optical disk according to a second embodiment of the present invention;

FIGS. 5A and 5B respectively present a cross section showing the optical system of a pickup which picks up information from the optical disk in FIG. 4 and a circuit diagram showing the electric circuit of this pickup;

FIGS. 6(a) to 6(d) are exemplary diagrams illustrating the arrangements of pits on the recording surface of an optical disk according to a third embodiment of the present invention;

FIGS. 7(a) to 7(d) are explanatory diagrams showing the intensity distributions of a reflected beam on the light-receiving surfaces of a photodetector when a read beam is irradiated on the pits arranged as shown in (a) to (d) in FIG. 6;

FIG. 8 is a circuit diagram showing a circuit to detect the pit arrangement;

FIG. 9 presents a characteristic diagram showing the relationship between the number of pits per unit and the number of wavelengths according to the third embodiment; and

FIG. 10 presents a characteristic diagram showing the relationship between the unit area density and the longest wavelength in use.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Preferred embodiments of the present invention will now be described referring to the accompanying drawings.

FIG. 1 is an exemplary diagram illustrating the arrangement of pits on the recording surface of an optical disk according to a first embodiment of the present invention.

In FIG. 1, a square unit area U is set in the circumferential direction of an optical disk or in the information recording direction R. The unit area U is divided into a first subunit U₁ and a second subunit U₂ with a center line L. The length U_P of each side of the unit area U represents the pitch between rows of pits or the pitch between tracks.

Pits P are provided in the first subunit U₁. The pits P have one of n depths (n: an integer equal to or greater than 2).

A read beam to be irradiated on an optical disk according to this invention forms a beam spot S_S of the shortest wavelength λ_S and a beam spot S_L of the longest wavelength λ_L.

The wavelengths of a plurality of components included in the read beam are respectively four times the n depths of the pits P. That is, with the wavelength of λ_n and the pits P having a depth of Δ_n, λ_n =4·Δ_n.

The length U_P of each side of the unit area U should be determined to be equal to or greater than λ_L /(2×NA) where NA is the number of apertures of the objective lens and the longest wavelength λ_L of beam components included in the read beam.

When the length U_P is set close to the cutoff frequency of the so-called OTF (Optical Transfer Function) of the pickup optical system, however, the level of the received light signal becomes smaller. In consideration of the wavelength characteristic of the output of the photodetector and a variation in the level of a beam component, it is preferable to set U_P to be about λ_L /(2^1/2 ×NA).

FIG. 2 illustrates an apparatus for reading information from a disk having such pits P.

In FIG. 2A, a laser beam source 10 emits a read beam 12 toward a polarization surface 13a of a polarization prism 13. The read beam 12 includes a plurality of frequency components f_n having wavelengths λ_n equal to four times the possible depths Δ_n of the pits P on an optical disk 11 of the present invention. In this embodiment, n=3. The read beam 12 passing the polarization surface 13a is irradiated on the recording surface of the optical disk 11 and is reflected therefrom. The reflected beam comes incident to the polarization surface 13a. As the polarization face of the reflected beam is changed due to the reflection, the reflected beam is reflected at the polarization surface 13a to be incident to a half mirror HM₁. This beam is separated into two reflected beam components. One of the reflected beam components enters a λ₁ -pass filter FL₁ which passes only a component of a wavelength λ₁, and the other component enters a half mirror HM₂. The λ₁ component that has passed the filter FL₁ enters a bisected photodetector D₁1.

The beam incident to the half mirror HM₂ is separated into two reflected beam components. One of the reflected beam components enters a λ₂ -pass filter FL₂ which passes only a component of a wavelength λ₂, and the other component enters a λ₃ -pass filter FL₃ which passes only a λ₃ component. The λ₂ component that has passed the filter FL₂ enters a bisected photodetector D₁2, while the λ₃ component that has passed the filter FL₃ enters a bisected photodetector D₁3.

As shown in FIG. 2B, each of the bisected photodetectors D₁1, D₁2 and D₁3 has light-receiving surfaces d₁ and d₂, and the light outputs of each photodetector are supplied to an associated differential amplifier DF₁, DF₂ or DF₃. The differential outputs of the individual differential amplifiers DF₁, DF₂ and DF₃ are supplied to one of the input terminals of NAND gates G₁, G₂ and G₃, respectively. The outputs of the bisected photodetector D₁3 also become input signals to a summing amplifier ADD whose output is one input signal of a comparator CP. As long as the input signal is lower than a reference voltage V_r, the comparator CP supplies a logic "0" signal to the other input terminals of the NAND gates G₁, G₂ and G₃. Upon reception of a low-level signal or a logic "0" signal at one input terminal from the differential amplifier DF₁, DF₂ or DF₂ while receiving the logic "0" signal at the other input terminal from the comparator CP, the NAND gate G₁, G₂ or G₃ outputs a logic "1" signal to an associated output terminal R₁, R₂ or R₃.

FIG. 3 presents a graph showing the relationship between the wavelength λ_n of the read beam to be irradiated on pits having a depth Δ_n and the levels of the output signals of the differential amplifiers DF₁, DF₂ and DF₃.

In FIG. 3, a solid line C₁1 shows a change in the level of the reflected beam when the read beam is irradiated on the pits P with a depth of 0.160 μm while the wavelength of the read beam is changed from 0.60 μm to 0.80 μm. A broken line C₁2 shows a change in the level of the reflected beam when the read beam is irradiated on the pits P with a depth of 0.175 μm while the wavelength of the read beam is changed from 0.60 μm to 0.80 μm. An alternate short and long dash line (phantom line) C₁3 shows a change in the level of the reflected beam when the read beam is irradiated on the pits P with a depth of 0.190 μm while the wavelength of the read beam is changed from 0.60 μm to 0.80 μm.

It is to be noted that 0 dB on the vertical scale corresponds to 30% of the incident amount of the read beam.

It is apparent from FIG. 3 that the output signal level of the differential amplifier DF_l corresponding to the wavelength λ₁ of 0.64 μm becomes zero or very small as indicated by the characteristic curve C₁1 for the pits P with a depth of 0.160 μm, the output signal level of the differential amplifier DF₂ corresponding to the wavelength λ₂ of 0.70 μm becomes zero or very small as indicated by the characteristic curve C₁2 for the pits P with a depth of 0.175 μm, and the output signal level of the differential amplifier DF₃ corresponding to the wavelength λ₃ of 0.76 μm becomes zero or very small as indicated by the characteristic curve C₁3 for the pits P with a depth of 0.190 μm.

But, the output signal level of the amplifier DF₁ becomes large for the pits P with a depth of 0.175 μm or 0.190 μm, the output signal level of the amplifier DF₂ becomes large for the pits P with a depth of 0.190 μm or 0.175 μm, and the output signal level of the amplifier DF₃ becomes large for the pits P with a depth of 0.160 μm or 0.175 μm.

Therefore, by irradiating one read beam including a plurality of wavelengths λ₁, λ₂ and λ₃ onto the pits P and separating the reflected beam into components for the individual wavelengths λ₁, λ₂ and λ₃ through the respective filters, the difference signal representing the difference between the outputs of the first and second bisected photodetector portions d₁ and d₂ is acquired for each wavelength component. It is understood that when the difference signal has a predetermined value or a logic "1", pits P with a depth of λ_n /4 corresponding to the wavelength λ_n of the read beam are not in the unit area U, and when the difference signal has a value of zero or a very small value, i.e., a logic "0", pits P with a depth of λ_n /4 corresponding to the wavelength λ_n of the read beam are in the unit area U.

According to the first embodiment, as apparent from the above, one information can be associated with one depth of the pits P, so that with n types of depths equal to or greater than 2 being set for the pits P, when the pits P are provided in one unit area U, this unit area can have two or more pieces of information. This can improve the information recording density.

FIG. 4 presents an exemplary diagram illustrating the arrangement of pits on the recording surface of an optical disk according to a second embodiment of the present invention. The same reference numerals as used in FIG. 1 are given to the corresponding or identical portions in FIG. 4 to avoid their redundant description.

For the optical disk shown in FIG. 4, the unit area U is divided in the circumferential direction and radial direction of the disk to be first to fourth subunits U₁1, U₁2, U₁3 and U₁4. First divided pits P₁ are located in the first subunit U₁1, and second divided pits P₂ in the second subunit U₁2. The first divided pits P₁ and second divided pits P₂ have any one of n depths (n: an integer equal to or greater than 2).

FIG. 5A shows the optical system of a pickup which detects information from the optical disk shown in FIG. 4, and FIG. 5B shows the electric circuit of this pickup.

The optical system in FIG. 5A has the same structure as the one shown in FIG. 2A except that it uses quadrant photodetectors D₂1, D₂2 and D₂3.

In the electric circuit shown in FIG. 5B, the received light signals from the light-receiving surfaces d₁, d₂, d₃ and d₄ of each quadrant photodetector D₂n are operated in differential amplifiers df₁ and df₂ to acquire a (d₁ -d₃) signal and a (d₂ -d₄) signal. The (d₁ -d₃) signal is supplied to one input terminal of a NAND gate g₁, and the (d₂ -d₄) signal is supplied to one input terminal of a NAND gate g₂. Summing amplifiers add₁ and add₂ respectively produce a (d₁ +d₃) signal and a (d₂ +d₄) signal and supply them to one input terminals of comparators CP₁ and CP₂. When the (d₁ +d₃) signal and (d₂ +d₄) signal fall below a reference voltage V_r, the comparators CP₁ and CP₂ output logic "0" signals. The outputs signals of the comparators CP₁ and CP₂ are respectively supplied to the other input terminals of the NAND gates g₁ and g₂. The NAND gate g₁ outputs a logic "1" on its output terminal r₁1 when the (d₁ -d₃) signal becomes a low level (logic "0") while the logic "0" signal is received from the comparator CP₁. The NAND gate g₂ outputs a logic "1" on its output terminal r₂1 when the (d₂ -d₄) signal becomes a low level (logic "0") while the logic "0" signal is received from the comparator CP₂.

The quadrant photodetectors D₂2 and D₂3 have the same circuit structure as the one shown in FIG. 5B and have outputs (r₁2, r₂2) and (r₁3, r₂3) though not shown. Therefore, a read beam with wavelengths of λ₁, λ₂ and λ₃ can provide a total of six pieces of information (r₁1, r₁2), (r₁2, r₂2) and (r₁3, r₂3) in a single unit area U.

Supposing that the pits P₁ and P₂ are respectively given two depths Δ₁ and Δ₂ corresponding to two wavelengths λ₁ and λ₂ for each unit area U on the optical disk shown in FIG. 4, at least four pieces of information can be recorded in each unit area by the combinations of the positional information of the pits P₁ and P₂ to the subunits U₁1 and U₁2. It is apparent that the information recording density can be improved.

In FIG. 6, (a) to (d) are exemplary diagrams illustrating the arrangement of pits on the recording surface of an optical disk according to a third embodiment of the present invention. The same reference numerals as used in FIGS. 1 and 4 are given to the corresponding or identical portions in FIG. 6 to avoid their redundant description.

FIG. 6(a) illustrates the case where the first divided pits P₁ are provided in the first subunit U₁1 and the second divided pits P₂ in the second subunit U₁2. FIG. 6(b) illustrates the case where the first divided pits P₁ are provided in the second subunit U₁2 and the second divided pits P₂ in the third subunit U₁3. FIG. 6(c) illustrates the case where the first divided pits P₁ are provided in the third subunit U₁3 and the second divided pits P₂ in the fourth subunit U₁4. FIG. 6(d) illustrates the case where the first divided pits P₁ are provided in the fourth subunit U₁4 and the second divided pits P₂ in the first subunit U₁1.

FIGS. 7(a) to 7(d) are explanatory diagrams showing the intensity distributions of a reflected beam on the light-receiving surfaces of a quadrant photodetector when a read beam is irradiated on the pits arranged as shown in (a) to (d) in FIG. 6.

FIG. 8 illustrates a detector that detects the pit arrangement.

In FIG. 8, the detector is connected to one (D₂1) of the quadrant photodetectors D₂1, D₂2 and D₂3 provided in the optical system of the pickup.

Summing amplifiers add₁, add₂, add₃ and add₄ output signals S₁ =(d₁ +d₂), S₂ =(d₂ +d₃), S₃ =(d₃ +d₄) and S₄ =(d₁ +d₄), respectively. A comparator CP₃ produces logic signals S_a, S_b, S_c and S_d corresponding to the four input signals S₁, S₂, S₃ and S₄. Each of the logic signals S_a, S_b, S_c and S_d will take a logical value of "1" when its one input signal is greater than the other input signal.

When the first divided pits P₁ are provided in the first subunit U₁1 and the second divided pits P₂ in the second subunit U₁2 as shown in (a) in FIG. 6, it is apparent from (a) in FIG. 7 that as the sum signal S₁ is the largest output among the sum signals S₁ to S₄, Sa=1 through the comparison of the sum signals S₁ to S₄ in the comparator CP₃. Sa=1 is the information representing that the first and second divided pits P₁ and P₂ are arranged as shown in (a) in FIG. 6.

Likewise, information representing the arrangement of the first and second divided pits P₁ and P₂ as shown in (b) to (d) in FIG. 6 can be obtained based on the result of the comparison done in the comparator CP₃.

According to the third embodiment of the present invention wherein the arrangement information of the first and second divided pits P₁ and P₂ are added to the second embodiment, one unit area U can have four times the amount of information available in the second embodiment, thus further improving the information recording density.

That is, pieces of information which correspond in number to the combinations of (S_a, S_b, S_c, S_d) and (r₁n, r₂n) can be recorded in a single unit area U.

FIG. 9 presents a characteristic diagram showing the relation between the number of pits per unit and the number of wavelengths (depths of pits) in the third embodiment.

FIG. 10 presents a characteristic diagram showing the unit area density and the longest wavelength in use.

In FIG. 10, a solid line C₂1 indicates the unit area density when the number of apertures NA is 0.45 and the longest wavelength λ_L ranges from 0.60 μm to 0.80 μm. A broken line C₂2 indicates the unit area density when the number of apertures NA is 0.50 and the longest wavelength λ_L ranges from 0.60 μm to 0.80 μm. An alternate long and short dash line C₂3 indicates the unit area density when the number of apertures NA is 0.55 and the longest wavelength λ_L ranges from 0.60 μm to 0.80 μm. An alternate long and two short dashes line C₂4 indicates the unit area density when the number of apertures NA is 0.60 and the longest wavelength λ_L ranges from 0.60 μm to 0.80 μm.

Next, the recording density will be described below.

Given that the number of wavelengths (depths of pits) is n in the third embodiment shown in FIG. 6, the number of combinations of the depths of the first and second divided pits P₁ and P₂ is expressed as follows.

number of combinations=(number of wavelengths)² ×4

The number of pits in those combinations is expressed as follows.

number of bits=log₂ (number of combinations)=log₂ [(number of combinations)² ×4]

Thus, the relationship between the number of pits per unit U and the number of wavelengths in the third embodiment becomes as shown in the characteristic diagram of FIG. 9.

The size of the unit U is determined by the longest wavelength λ_L and is given by the following equation.

unit size=[λ_L /(2^1/2 ×NA)]²

Thus, the relationship between the longest wavelength χ_L and the unit density becomes as shown in FIG. 10.

From the above, the recording density in the third embodiment is given as follows.

recording density={log₂ [number of combinations)² ×4]}/[λ_L /(2^1/2 ×NA)]²

When the longest wavelength λ_L is 0.785 μm which is the wavelength of the existing pickup, the number of wavelengths is 2 and the number of apertures NA is 0.5 which is the same as the existing one, the recording density becomes 0.8×4=3.2 (pits/μm²), 2.4 times that of the existing CD, from the above equation.

A sync signal may be recorded on the optical disk by inserting a sync pit within a group of consecutive pits and the sync signal can be utilized for detecting a timing when the reading spot coincide with the unit area. The information signal based on the reflected beam may be evaluated at each of the particular sync timings.

In short, the optical disk according to the present invention has pit information recorded by setting multi-leveled depths for the pits provided in individual unit areas continuously segmented in the information recording direction, so that the information recording density can be improved.

According to the optical-disk information reproducing method of the present invention, a beam having a plurality of wavelengths corresponding to four times the multi-leveled depths of pits is irradiated as a read beam to each unit area on the optical disk, pit information is acquired based on the reflected beam from the unit area, and composite pit information recorded on the optical disk is reproduced based on the combination of the arrangement information of the pits in the unit area and the depth information of the pits.

Claims

1. An information reproducing method of reproducing information from an optical disk having unit areas continuously provided in a circumferential direction, each bit of said information being recorded in the form of a pit, wherein said optical disk comprises at least one pit in each of said unit areas, said pit having a depth of one of n depths, n being an integer having a value of at least two, wherein each bit of said information recorded in the form of a pit has a depth which corresponds respectively to one of said n depths, each bit of said information being recorded by setting a depth of a corresponding pit, said information reproducing method comprising the steps of:

irradiating a read beam having frequency components of n wavelengths corresponding to four times said n depths, respectively, to a row of said unit areas; and

acquiring pit information based on an intensity distribution in a plane perpendicular to an optical axis of a reflected beam from said row of unit areas.

2. An information reproducing method of reproducing information from an optical disk having unit areas continuously provided in a circumferential direction, each bit of said information being recorded in the form of a pit, wherein said optical disk comprises at least one pit in each of said unit areas, said pit having a depth of one of n depths, n being an integer having a value of at least two, wherein each bit of said information recorded in the form of a pit has a depth which corresponds respectively to one of said n depths, each bit of said information being recorded by setting a depth of a corresponding pit, and wherein each of said unit areas is divided in a circumferential direction into at least two sub areas arranged in a radial direction of said disk, at least one of said two sub areas comprising one pit corresponding to at least one bit, said information reproducing method comprising the steps of:

irradiating a read beam having frequency components of n wavelengths corresponding to four times said n depths, respectively, to a row of said unit areas;

acquiring pit information for each of said sub areas based on an intensity distribution in a plane perpendicular to an optical axis of a reflected beam from said row of unit areas; and

acquiring composite pit information from a combination of said pit information for said sub areas.

3. An information reproducing method of reproducing information from an optical disk having unit areas continuously provided in a circumferential direction, each bit of said information being recorded in the form of a pit, wherein said optical disk comprises at least one pit in each of said unit areas, said pit having a depth of one of n depths, n being an integer having a value of at least two, wherein each bit of information recorded in the form of a pit has a depth which corresponds respectively to one of said n depths, each bit of said information being recorded by setting a depth of a corresponding pit, and wherein each of said unit areas is divided in a circumferential direction into at least two sub areas arranged in a radial direction of said disk, at least one of said two sub areas comprising one pit corresponding to at least one bit, wherein each of said unit areas is further divided into two in a radial direction of said disk to provide four sub areas, wherein said pit is divided into two divided pits, said divided pits being arranged in any two of said four sub areas, said information reproducing method comprising the steps of:

irradiating a read beam having frequency components of n wavelengths corresponding to four times said n depths, respectively, to a row of said unit areas;

acquiring distribution information of said two divided pits in said four sub areas and divided-pit information of said two divided pits based on an intensity distribution in a plane perpendicular to an optical axis of a reflected beam from said row of unit areas; and

acquiring composite pit information from a combination of said distribution information of said two divided pits and said divided-pit information for every said two divided pits.